Table REF  lists the presently calculated \(E2\)  and \(M1\)  matrix elements for some important transitions and some available theoretical results [1]}, [2]}, [3]}. The \(M1\)  matrix elements are very small, about 10\(^{-4}\)  \(\sim \)  10\(^{-6}\) , except for the \(2s2p~^3P_0 \rightarrow 2s2p~^3P_1\)  transition. The present RCICP results agree very well with the other theoretical results [1]}, [3]}. The differences are less than 2%. For the \(2s2p~^3P_0 \rightarrow 2s2p~^3P_1\)  transition, the \(M1\)  matrix element are four to six orders of magnitude larger than the \(M1\)  matrix elements of the other \(M1\)  transitions. For the \(E2\)  matrix elements, we only found two available theoretical data [1]}, [3]}, that is for the \(2s^2~^1S_0 \rightarrow 2s3d~^1D_2\)  and \(2s2p~^3P_0 \rightarrow 2s2p~^3P_2\)  transitions, to compare with the present results. The present RCICP results agree very well with these two results, and the difference is no more than 1%.
